Unterschiede
Hier werden die Unterschiede zwischen zwei Versionen angezeigt.
| Beide Seiten der vorigen RevisionVorhergehende ÜberarbeitungNächste Überarbeitung | Vorhergehende Überarbeitung | ||
| en:berechnungen:festigkeitsberechnung [2025/02/18 09:33] – cschall | en:berechnungen:festigkeitsberechnung [2025/09/03 12:27] (aktuell) – [Shear Stress] neelest | ||
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| ======Stress Analysis====== | ======Stress Analysis====== | ||
| - | The strength calculation determines the maximum load of the screw with the shear | + | -> [[..: |
| - | stress hypothesis according to TRESCA: | + | |
| + | ===== Equivalent Stress===== | ||
| + | |||
| + | The strength calculation determines the maximum load on the screw using the shear stress hypothesis according to TRESCA: | ||
| $$σ_v = \sqrt {(σ_x - σ_y)^2 + 4τ_{xy}^2}$$ | $$σ_v = \sqrt {(σ_x - σ_y)^2 + 4τ_{xy}^2}$$ | ||
| - | The screw fails above this stress. The hypothesis | + | Since the rotation of the screw represents a purely torsional load, the hypothesis |
| - | of the screw generates only torsion stress, neither bend nor normal | + | As bending |
| - | therefore just shear stress | + | $\sigma_y$ may likewise be disregarded. |
| - | calculated according to the following formula: | + | The normal |
| - | $$τ_{nominal} | + | $$σ_v = \sqrt {σ_x^2 + 4τ_{xy}^2}$$ |
| - | with the torque | + | The screw' |
| - | Another influencing factor for the calculation of the screw strength is the radius, which | + | ===== Normal Stress===== |
| - | indicates the transition from the bottom of the screw to the flight; a shape number is | + | |
| - | defined for this geometric influence: | + | |
| - | $$\alpha_\tau = 1+ \frac{1}{\sqrt{3,4 \cdot \frac{r}{t} + 38 \cdot \frac {r}{d} (1+ 2 \cdot \frac{r}{d})^2 + (\frac{r}{d})^2 \cdot \frac{d}{D}}}$$ | + | The normal stress in the x-direction within the screw results from the pressures at the beginning and end of the screw. In this context, the pressure at the hopper generally plays a minor role and is usually only relevant for melt extruders. |
| - | with the radius at the flight | + | $$\sigma_x = \sigma_{x,Hopper} + \sigma_{x, |
| + | $$\text{with}$$ | ||
| + | $$\sigma_{x, | ||
| + | $$\text{and}$$ | ||
| + | $$\sigma_{x, | ||
| - | Together | + | With the outer diameter $D$ and the screw core diameter $d$.\\ |
| + | The acting force results from the pressure and the projected area on which the pressure acts. It is assumed that the compressive stress is transmitted solely through the screw core. | ||
| + | |||
| + | ===== Shear Stress===== | ||
| + | |||
| + | The shear stress resulting from the applied torque is calculated using the following formula: | ||
| + | |||
| + | $$\tau_{nominal} = \frac{M_t}{W_t} = \frac{M_t \cdot a_{max}}{I_p}$$ | ||
| + | |||
| + | with the torque $M_t$, the section modulus $W_t$, the polar moment of inertia $I_p$ and the maximum perpendicular distance from the outer fiber to the neutral (stress-free) fiber $a_{max}$. | ||
| + | |||
| + | Another influencing factor for calculating the screw strength is the radius that describes the transition from the screw core to the flight. For this geometric influence, a shape factor (stepped round bar under torsion, DIN 743-2) is defined as: | ||
| + | |||
| + | $$\alpha_{\tau} = 1+ \frac{1}{\sqrt{3, | ||
| + | |||
| + | with the radius at the flight $r$, the radius difference $t = \frac{D}{2} - \frac{d}{2} = h$, the screw core diameter $d$ and the outer diameter $D$. | ||
| + | |||
| + | From the shape factor, | ||
| $$\beta_{\tau} = \frac{\alpha_\tau}{n}$$ | $$\beta_{\tau} = \frac{\alpha_\tau}{n}$$ | ||
| $$\text{with}$$ | $$\text{with}$$ | ||
| - | $$n=1+\sqrt{G' | + | $$n=1+\sqrt{G' |
| $$\text{and}$$ | $$\text{and}$$ | ||
| $$G' | $$G' | ||
| - | the total influence factor $K_\tau$ | + | The total influence factor $K_\tau$ (DIN 743-1) |
| $$K_\tau = \left( \frac{\beta_\tau}{K_2(d)}+\frac{1}{K_{F, | $$K_\tau = \left( \frac{\beta_\tau}{K_2(d)}+\frac{1}{K_{F, | ||
| $$\text{with}$$ | $$\text{with}$$ | ||
| - | $$K_2(d)=1-0, | + | $$K_2(d)=1-0, |
| - | + | ||
| - | and with the influence of the surface roughness $K_{F, | + | |
| - | + | ||
| - | The stress occurring under consideration of the influencing factors results in: | + | |
| - | + | ||
| - | $$τ_{max}=τ_{nominal} \cdot K_\tau$$ | + | |
| - | The screw stability is given if | + | as well as with the influence of surface roughness $K_{F, |
| + | The values apply up to a diameter of 25 mm and decrease linearly beyond this value down to 1.0 at a diameter of 40 mm. For diameters above 40 mm, the value remains constant at 1.0. | ||
| - | $$\tau_{max} < \tau__{permissible}$$ | + | The resulting shear stress, taking into account these influencing factors, is given by: |
| - | The permissible shear stress | + | $$\tau_{xy} = \tau_{max}=\tau_{nominal} \cdot K_\tau$$ |
| ===Further topics=== | ===Further topics=== | ||
| * [[en: | * [[en: | ||
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